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To understand the molecular basis and to prevent diseases such as Alzheimer's disease (AD), the targets of the triggering agent have to be elucidated. beta-Amyloid peptide (Abeta) is the major component of extracellular senile plaques characteristic of AD. For a very long time, the aggregated form of the Abeta was supposed to be responsible for the neurodegeneration that occurs in AD. Recently, the attention has been diverted to the monomeric or oligomeric forms of Abeta and their interaction with cellular targets. In our investigation, the physiological and medically important insertion of externally applied Abeta monomers into the bilayer of lipid vesicles is demonstrated. Abeta(25-35) has been localized in the region of the lipid alkyl chain, and it has a severe disordering effect on the lamellar order of the lipid bilayer. Both of these results are of biomedical relevance.

The small G protein adenosine diphosphate ribosylation factor-1 (ARF1) is activated by cell membrane binding of a self-folding N-terminal domain. We present a model of the human ARF1 N-terminal peptide in planar lipid bilayers, determined from neutron lamellar diffraction and circular dichroism data with molecular modelling. This amphipathic domain lies at a shallow membrane depth, ideal for regulation of the ARF1 bio-timer by rapid, reversible membrane binding. The helical region does not elongate upon membrane binding, leaving the connecting flexible linker region's length unchanged.

It has been shown that water molecules participate in the proton pathway of bacteriorhodopsin. Large efforts have been made to determine with various biophysical methods the number of water molecules involved. Neutron diffraction H2O/D2O exchange experiments have been often used to reveal the position of water even with low-resolution diffraction data. With this technique, care must be taken with the limitations of the difference Fourier method which are commonly applied to analyze the data. In this paper we compare the results of the difference Fourier method applied to measured diffraction data (not presented here) and models with those from alternative methods introduced here: (1) a computer model calculation procedure to determine a label's scattering length density based on a comparison of intensity differences derived from models and intensity differences from our measurements; (2) a method based on the Parseval formula. Both alternative methods have been evaluated and tested using results of neutron diffraction experiments on purple membranes (Hauss et al. 1994). Our findings indicate that the difference Fourier method applied to low-resolution diffraction data can successfully determine the position of localized water molecules but underestimates their integrated scattering length density in the presence of labels in other positions. Furthermore, we present the results of neutron diffraction experiments on purple membranes performed to determine the number of water molecules in the projected area of the Schiff base at 86%, 75% and 57% relative humidity (r.h.). We found 19 +/- 2 exchangeable protons at 75% r.h., which means at least 8-9 water molecules are indispensable for normal pump function.

A recently proposed model for proton leakage across biological membranes [Prog. Lipid Res. 40 (2001) 299] suggested that hydrocarbons specifically in the center of the lipid bilayer inhibit proton leaks. Since cellular membranes maintain a proton electrochemical gradient as a principal energy transducer, proton leakage unproductively consumes cellular energy. Hydrocarbons in the bilayer are widespread in membranes that sustain such gradients. The alkaliphiles are unique in that they contain up to 40 mol% isoprenes in their membranes including 10-11 mol% squalene [J. Bacteriol. 168 (1986) 334]. Squalene is a polyisoprene hydrocarbon without polar groups. Localizing hydrocarbons in lipid bilayers has not been trivial. A myriad of physical methods including fluorescence spectroscopy, electron-spin resonance, nuclear magnetic resonance as well as X-ray and neutron diffraction have been used to explore this question with various degrees of success and often contradictory results. Seeking unambiguous evidence for the localization of squalene in membranes or lipid bilayers, we employed neutron diffraction. We incorporated 10 mol% perdeuterated or protonated squalane, an isosteric analogue of squalene, into stacked bilayers of dioleoyl phosphatidyl choline (DOPC) doped with dioleoyl phosphatidyl glycerol (DOPG) to simulate the negative charges found on natural membranes. The neutron diffraction data clearly show that the squalane lies predominantly in the bilayer center, parallel to the plane of the membrane.

Neuronal plasma membranes are thought to be the primary target of the neurotoxic beta-amyloid peptides (Abeta) in the pathogenesis of the Alzheimer's disease. Histologically, Abeta peptides are observed as extracellular macroscopic senile plaques, and most biophysical techniques have indicated the presence of Abeta close to the lipid headgroup region but not in the core of the membrane bilayers. The focus of this study is an investigation of the interaction between Abeta and lipid bilayers from a structural point of view. Neutron diffraction with the use of selectively deuterated amino acids has allowed us to determine unambiguously the position of the neurotoxic fragment Abeta (25-35) in the membrane. Two populations of the peptide are detected, one in the aqueous vicinity of the membrane surface and the second inside the hydrophobic core of the lipid membrane. The location of the C terminus was studied in two different lipid compositions and was found to be dependent on the surface charge of the membrane. The localization of beta-amyloid peptides in cell membranes will offer new insights on their mechanism in the neurodegenerative process associated with Alzheimer's disease and might provide clues for therapeutic developments.

Neutron diffraction has been used to study the membrane-bound structure of substance P (SP), a member of the tachykinin family of neuropeptides. The depth of penetration of its C-terminus in zwitterionic and anionic phospholipid bilayers was probed by specific deuteration of leucine 10, the penultimate amino acid residue. The results show that the interaction of SP with bilayers, composed of either dioleoylphosphatidylcholine (DOPC), or a 50:50 mixture of DOPC and the anionic phospholipid dioleoylphosphatidylglycerol (DOPG), takes place at two locations. One requires insertion of the peptide into the hydrophobic region of the bilayer, the other is much more peripheral. The penetration of the peptide into the hydrophobic region of the bilayer is reflected in a marked difference in the water distribution profiles. SP is seen to insert into DOPC bilayers, but a larger proportion of the peptide is found at the surface when compared to the anionic bilayers. The positions of the two label populations show only minor differences between the two types of bilayer.

Bimetallic, oxalate-bridged compounds with bi- and trivalent transition metals comprise a class of layered materials which express a large variety in their molecular-based magnetic behavior. Because of this, the availability of the corresponding single-crystal structural data is essential to the successful interpretation of the experimental magnetic results. We report in this paper the crystal structure and magnetic properties of the ferromagnetic compound {[N(n-C(3)H(7))(4)][Mn(II)Cr(III)(C(2)O(4))(3)]}(n)() (1), the crystal structure of the antiferromagnetic compound {[N(n-C(4)H(9))(4)][Mn(II)Fe(III)(C(2)O(4))(3)]}(n)() (2), and the results of a neutron diffraction study of a polycrystalline sample of the ferromagnetic compound {[P(C(6)D(5))(4)][Mn(II)Cr(III)(C(2)O(4))(3)]}(n)() (3). Crystal data: 1, rhombohedral, R3c, a = 9.363(3) Å, c = 49.207(27) Å, Z = 6; 2, hexagonal, P6(3), a = 9.482(2) Å, c = 17.827(8) Å, Z = 2. The structures consist of anionic, two-dimensional, honeycomb networks formed by the oxalate-bridged metal ions, interleaved by the templating cations. Single-crystal field dependent magnetization measurements as well as elastic neutron scattering experiments on the manganese(II)-chromium(III) samples show the existence of long-range ferromagnetic ordering behavior below T(c) = 6 K. The magnetic structure corresponds to an alignment of the spins perpendicular to the network layers. In contrast, the manganese(II)-iron(III) compound expresses a two-dimensional antiferromagnetic ordering.